Euler Singularities I: Boundary Blow-Up for Smooth Exact-Odd Axisymmetric Euler with Swirl

Abstract

We construct smooth axisymmetric-with-swirl initial data in a periodic cylinder for which the three-dimensional incompressible Euler evolution develops a finite-time boundary singularity. The construction is carried out in the dynamically invariant exact-odd class \[ (r,-z,t)=-(r,z,t), G(r,-z,t)=-G(r,z,t), \] where \(=r uθ\) and \(G=ωθ/r\). At the side-wall point \((r,z)=(1,0)\), exact oddness gives the pointwise identities \[ ∂t∂zG(1,0,t) = σ(t)∂zG(1,0,t) +2(∂z(1,0,t))2, ∂t∂z(1,0,t) = σ(t)∂z(1,0,t), \] with \(σ(t)=-∂z uz(1,0,t)\). The proof is based on a side-wall Dirichlet parametrix for the five-dimensional lifted recovery equation \(-5φ=G\). Near the wall, the effective compression kernel has leading term \[ K0(x,y)=C0xy(x2+y2)2, C0>0, \] with controlled remainders, parity-based shear cancellation, and strain-variation bounds on narrow diagonal cones. These estimates are combined with an over-compressed dyadic angular cluster functional. The cluster functional absorbs same-scale angular fragmentation, growing dyadic windows, dynamically separated far tails, and fixed-distance exterior fields into an integrably small affine Campanato defect. The resulting invariant cluster contains a uniformly coherent component with amplitudes \(A*(t)\) and \(B*(t)\) satisfying the Dini comparison system \[ D+A*(t) cB*(t)2, D+B*(t) cA*(t)B*(t). \]

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